TY - JOUR
T1 - Magnetic glass in shape memory alloy
T2 - Ni 45Co 5Mn 38Sn 12
AU - Lakhani, Archana
AU - Banerjee, A.
AU - Chaddah, P.
AU - Chen, X.
AU - Ramanujan, R. V.
PY - 2012/9/26
Y1 - 2012/9/26
N2 - The first order martensitic transition in the ferromagnetic shape memory alloy Ni 45Co 5Mn 38Sn 12 is also a magnetic transition and has a large field induced effect. While cooling in the presence of a field this first order magnetic martensite transition is kinetically arrested. Depending on the cooling field, a fraction of the arrested ferromagnetic austenite phase persists down to the lowest temperature as a magnetic glassy state, similar to the one observed in various intermetallic alloys and in half doped manganites. A detailed investigation of this first order ferromagnetic austenite (FM-A) to low magnetization martensite (LM-M) state transition as a function of temperature and field has been carried out by magnetization measurements. Extensive cooling and heating in unequal field (CHUF) measurements and a novel field cooled protocol for isothermal MH measurements (FC-MH) are utilized to investigate the glass like arrested states and show a reverse martensite transition. Finally, we determine a field-temperature (HT) phase diagram of Ni 45Co 5Mn 38Sn 12 from various magnetization measurements which brings out the regions where thermodynamic and metastable states coexist in the HT space, clearly depicting this system as a magnetic glass.
AB - The first order martensitic transition in the ferromagnetic shape memory alloy Ni 45Co 5Mn 38Sn 12 is also a magnetic transition and has a large field induced effect. While cooling in the presence of a field this first order magnetic martensite transition is kinetically arrested. Depending on the cooling field, a fraction of the arrested ferromagnetic austenite phase persists down to the lowest temperature as a magnetic glassy state, similar to the one observed in various intermetallic alloys and in half doped manganites. A detailed investigation of this first order ferromagnetic austenite (FM-A) to low magnetization martensite (LM-M) state transition as a function of temperature and field has been carried out by magnetization measurements. Extensive cooling and heating in unequal field (CHUF) measurements and a novel field cooled protocol for isothermal MH measurements (FC-MH) are utilized to investigate the glass like arrested states and show a reverse martensite transition. Finally, we determine a field-temperature (HT) phase diagram of Ni 45Co 5Mn 38Sn 12 from various magnetization measurements which brings out the regions where thermodynamic and metastable states coexist in the HT space, clearly depicting this system as a magnetic glass.
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U2 - 10.1088/0953-8984/24/38/386004
DO - 10.1088/0953-8984/24/38/386004
M3 - Article
AN - SCOPUS:84866121042
SN - 0953-8984
VL - 24
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 38
M1 - 386004
ER -